Once the probability is properly defined, we can calculate it in different models of the modified LQCs. In LQC [1]}, the calculations were carried out for the quadratic potential.
In order to compare the results obtained in different models, let us consider the same potential. Then, for the mLQC-I model it was found that [2]}
\(&& \sin \left(\lambda b_B^{\scriptscriptstyle {\mathrm {I}}}\right)=\sqrt{\frac{1}{2\gamma ^2+2}}, \quad \sin \left(2\lambda b_B^{\scriptscriptstyle {\mathrm {I}}}\right)=\frac{\sqrt{2\gamma ^2+1}}{\gamma ^2+1},\nonumber \\&& p^{\scriptscriptstyle {\mathrm {I}}}_\phi =v\left(2\rho ^{\scriptscriptstyle {\mathrm {I}}}_c-2 V\right)^{\frac{1}{2}}, \quad d\omega ^{\scriptscriptstyle {\mathrm {I}}}=\left(2\rho ^{\scriptscriptstyle {\mathrm {I}}}_c-2 V\right)^{\frac{1}{2}} d\phi , ~~~~~~~~\) 
